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8 Jan 2018: Nonlinear NonmodalStability Theory. R. R. Kerswell,School of Mathematics, Bristol University, Bristol, U.K., BS8 1TW; email:. R.R.Kerswell@bris.ac.uk. Xxxx. Xxx. Xxx. Xxx. YYYY. AA:1–30. This article’s doi:. 10.1146/((please add article doi)).

13 Dec 2018: For scalar wave fields witharbitrary incident angles the scattered field obeys the Helmholtzboundary integral equation [1, 24]. ... Sel. Top. Appl. Earth Obs. Remote. Sens. 7,1573–1583 (2014). 24. J.

13 Dec 2018: T ′ij = lipljqTpq (3.24). can be rewritten in matrix notation as T ′ = LT LT – check this yourself!

23 Jan 2018: qq′). (1.24). Upon the substitution p′ = p m(qq′). t this becomes. ... Z0[J] =. d[ϕ] e. i2. ddx (µϕ(x)µϕ(x)m. 2ϕ2(x))iddx J(x)ϕ(x). (2.24). This is an integral with a highly oscillating integrand; if

13 Dec 2018: This is precisely our archetypal variational. problem with. f(x,y,y′) =. 1 y′2, (1.24). ... NST IB Mathematical Methods II 24. case of the adjustable parameters, then the Rayleigh–Ritz method will find both y0 and.

14 May 2018: S[a] =. Z1. 2ab @. µa@µb. m2. 2ab. ab (ab ab)2 ddx (6.24).

25 Oct 2018: f 0(xi)|,. (6.24). where the first equality used equation (6.21) and the second (6.22).

18 Nov 2018: Doyle and C. McMullen [24]: “But can be solved in the case ofthe quartic and the quintic using several limits (towers of generallyconvergent iterative maps linked serially).”. ... P. Doyle and C. McMullen [24]: “But can be solved in the case ofthe

26 Apr 2018: There are also a number of excellent books, and Google returns about 24,300,000 hits for the search‘Matlab introduction’ (up from 13,400,000 hits last year), and about